Coulomb gluons and colour evolution

Transcription

1 Coulomb gluons and colour evolution René Ángeles-Martínez in collaboration with Jeff Forshaw Mike Seymour JHEP 1512 (2015) 091 & arxiv: (accepted for publication) 1 DPyC, BUAP 2016

2 In this talk: Progress towards including the colour interference of soft gluons in partons showers. PDF Hard process (Q) Parton Shower: Approx: Collinear + Soft radiation Q q µ QCD Underlying event Hadron-Hadron collision, Soper (CTEQ School) Hadronization 2

3 Motivation Why? Increase precision of theoretical predictions for the LHC Is this necessary? Yes, for particular non-inclusive observables. Are those relevant to search for new physics? Yes, these can tell us about the (absence of) colour of the production mechanism (couplings). 3

4 Outline Coulomb gluons, collinear factorisation & colour interference. Concrete effect: super-leading-logs. Including colour interference in partons showers. (Also see JHEP 07, 119 (2015), arxiv: & ) 4

5 One-loop in the soft approximation k µ Q ij Colour matrices acting on ig 2 st i T j Z d d k (2 ) d 2 Hard subprocess is a vector colour + spin p i p j [p j k±i0][ p i k±i0][k 2 +i0] 2 i : j : i0 i0 i : +i0 j : +i0 5 i : i0 j : +i0

6 Introduction: one-loop soft gluon correction After contour integration: g 2 sµ 2 T i T j p i p j Z d 4 k (2 ) 4 apple (2 ) (k 2 ) (k 0 ) [p j k][p i k] + i ij (2 ) 2 (p i k) ( p j k) 2[k 2 ] 2 (On-shell gluon: Purely real) (Coulomb gluon: Purely imaginary) ij = 8 >< 1 if i, j in, 1 if i, j out, >: 0 otherwise. 6

7 Tree-level collinear factorisation For a general on-shell scattering: Colour + Spin operator. Depends only on collinear partons Depends only on non-collinear partons 7

8 Generalised factorisation beyond tree level Catani, De Florian & Rodrigo JHEP 1207 (2012) 026 This collinear factorisation generalises to all orders but Violation of strict (processindependent) factorisation! 8

9 Generalised factorisation: one loop The problem first seed at this order 9

10 Breakdown of color coherence Effectively, correction to 10

11 Breakdown of color coherence Effectively, correction to Unavoidable colour correlation 10

12 Coulomb gluons and (the lack of) coherence Conclusion: coherence allows us to unhook on-shell gluons and recover process independent factorisation. But it fails for Coulomb gluons. instead of Can we make sense of these nested structure? 11

13 Concrete case: gaps-between-jets ( Forshaw, Kyrieleis & Seymour hep / ; / ) Y/2, Y/2, inside the gap q T <Q 0 Q Q Q Any q T Q Q Q 0 outside the gap m = Soft corrections Z M(q 1,...,q m ) 2 dps Q 0 q i Q (On-shell gluons) Q s n ln n 2 Q 2 0 Super-leading logs (On-shell + Coulomb gluons) Q s 3 ln 4 2 Q, s 4 ln 5 2 Q 2 0 Q Origin: lack of coherence (strict factorisation).

14 Parton showers (Produce events from approximate x-sections) Typically: - X-section approximated by ordering real radiation - Soft radiation included but no colour interference. - Virtual radiation included indirectly via unitarity. 13

15 Parton showers (Produce events from approximate x-sections) Typically: - X-section approximated by ordering real radiation - Soft radiation included but no colour interference. - Virtual radiation included indirectly via unitarity. Colour interference: - Ansatz (hep / ): Order soft radiation, real & virtual, according to its hardness. - Is the specific ordering variable relevant? 13

16 The role of the ordering variable is crucial! (Banfi, Salam, Zanderighi JHEP06(2010)038) The coefficients of super-log varies for different ordering variables: - Angular ordering: zero. - Energy ordering: infinite. - Transverse momentum ordering: finite. - Virtuality ordering: 1/2. Our strategy to solve this problem: Brute force! Eikonal approximation Exact 3 & 4 -gluon vertex & ghosts Complete (1-loop) diagrammatic calculation assuming that all gluons are soft, but not relatively softness (RAM, Forshaw, Seymour: PhD thesis, JHEP 1512 (2015) 091 & arxiv: ) 14

17 Coulomb gluons and colour evolution Our fixed order calculations suggest that the one-loop amplitude of a general hard scattering with N soft-gluon emissions (ordered in softness q i q i+1 )is E n (1) N + NX m=1 = NX m=0 n+m X 1 j=1 px i=2 Xi 1 j=1 n+m X 1 k=1 J (0) (q N ) J (0) (q m+1 ) I ij (q (ij) m+1,q(ij) m )J (0) (q m ) J (0) (q 1 ) n (0) 0 i J (0) (q N ) J (0) (q m+1 ) I n+m,j (q (ij) m+1,q(jk) m ) d jk (q m )J (0) (q m 1 ) J (0) (q 1 ) n (0) 0 i, where the virtual insertion operator: I ij (a, c) =I ij (a, b)+i ij (b, c) describes the non-emission evolution of partons i and j from a to c. q µ = p µ i + pµ j +(q(ij) T )µ Key point: The Ordering variable is dipole kt 15 - Gauge invariant. - Correct IR poles - Interpretation: ordered evolution! -

18 Sketch in the simplest case Decomposition in colour and spin i.e. non-trivial test of k_t ordering! 16

19 Diagrammatics of dipole: kt ordering 1.- Add N-emissions on external legs 2.- Add virtual exchanges Case a) Case b) 17

20 Diagrammatics of dipole: kt ordering 1.- Add N-emissions on external legs 2.- Add virtual exchanges Case a) Case b) a) b) and apply effective rules: Gauge invariance 17

21 Non-emission evolution operator On-shell Coulomb I ij (a, b) = s 2 T i T j c Z d(k (ij) ) 2 (k (ij) ) ln p Z2p + i /kij ln p 2p j /k ij dy p i p j 2[p j k][p i k] i ij (k (ij) ) (a <k (ij) <b) This is the same one-loop operator that appears at one-loop but kt ordered! k µ = p µ i + pµ j +(k(ij) ) µ 18

22 Diagrammatics of dipole kt evolution For a general scattering n we need spheres The effective rules are the same: 19

23 Summary / Conclusion Coulomb gluons introduce colour-interference & play an essential role in the evolution of hard processes: super-leading logs violations of coherence Can be incorporated at amplitude level as an evolution in dipole transverse momentum, making sense of Future: Monte Carlo Parton Shower for general observables. 20